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Year 13 Momentum - Rogue Physicist
Year 13 Momentum - Rogue Physicist

... which is initially at rest. The collision is inelastic such that they join and move away with a common velocity. a) What is the initial momentum of each mass? b) By applying the principal of conservation of momentum, find the velocity with which the masses move away. c) Show that the momentum before ...
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Physics of Motion Lecturer:  Mauro Ferreira
Physics of Motion Lecturer: Mauro Ferreira

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Applying conservation of momentum: collisions.

Ch 13 Equilibrium
Ch 13 Equilibrium

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... Old Grandma Jones is trying to load a wooden crate full of apples into her truck. To accomplish this, she plans to slide the crate up along a board. If the crate has a mass of 50 kg and the board is at a 30º incline, what is the maximum force she must apply parallel to the board to move the crate at ...
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Sliders – High School Worksheet

... 11. For each trial, calculate the speed the basket was moving right before it hit the floor. Use the kinematics equations to solve: d = (vi + vf)/2 * t The basket started at rest so the initial velocity is zero. By plugging in the measured values, we can calculate the final velocity. 0.21 m = vf / 2 ...
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... Yes, the direction of velocity is changing. Centripetal acceleration is provided by the tension in the string. The centripetal acceleration is different in the two cases presented, therefore, the tension will be different Note that the radius has not changed in the two conditions Note also that angu ...
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... future. Objects only know what is acting directly on them right now Newton's 1st Law An object that is at rest will remain at rest and an object that is moving will continue to move in a straight line with constant speed, if and only if the sum of the forces acting on that object is zero. Newton's 3 ...
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... second law for the acceleration of the center of mass and the rotational analog of Newton’s second law for the angular acceleration about the center of mass. • Follow Example 10.6 using Figure 10.18. ...
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Kepler`s Laws Adobe Acrobat

... hand side of (2) is 0. It follows that the vector h=r×v is constant. We conclude that both the position and velocity vector lie in a plane normal to h. Choose coordinates so that this plane is the xy-plane. Then h = hk for some constant scaler h. (We have assumed h 6= 0; in case h = 0 it can be show ...
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LECTURE 27: Gravitational potential energy

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LECTURE 27: Gravitational potential energy

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An Equivalent Electrical Model for Numerical Analyses of ODEP

... where υ is the particle velocity, u the liquid velocity, Fd the drag force and fr the friction factor of the particle in the fluid. For a spherical particle fr = 6πηR, where η is the dynamic viscosity of the medium. Assuming that the liquid velocity can be neglected because the initial condition of ...
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Lecture Outline - UIC Department of Physics
Lecture Outline - UIC Department of Physics

work is also defined as `the product of displacement and the force in
work is also defined as `the product of displacement and the force in

Classical Mechanics - Mathematical Institute Course Management
Classical Mechanics - Mathematical Institute Course Management

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... (a) What is the maximum speed of that point in SI units? (b) What is the maximum acceleration of the point in SI units? Answer: (a) 6.82 m/s (b) 3.75 × 104 m/s2 4) A ball is oscillating on an ideal spring with an amplitude of 8.3 cm and a period of 4.6 s. Write an expression for its position, x, as ...
PPTX
PPTX

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Classical central-force problem



In classical mechanics, the central-force problem is to determine the motion of a particle under the influence of a single central force. A central force is a force that points from the particle directly towards (or directly away from) a fixed point in space, the center, and whose magnitude only depends on the distance of the object to the center. In many important cases, the problem can be solved analytically, i.e., in terms of well-studied functions such as trigonometric functions.The solution of this problem is important to classical physics, since many naturally occurring forces are central. Examples include gravity and electromagnetism as described by Newton's law of universal gravitation and Coulomb's law, respectively. The problem is also important because some more complicated problems in classical physics (such as the two-body problem with forces along the line connecting the two bodies) can be reduced to a central-force problem. Finally, the solution to the central-force problem often makes a good initial approximation of the true motion, as in calculating the motion of the planets in the Solar System.
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